Search results for "Zero-point energy"

showing 10 items of 20 documents

Zero‐Energy Rotating Accretion Flows near a Black Hole

1996

We characterize the nature of thin, axisymmetric, inviscid, accretion flows of cold adiabatic gas with zero specific energy in the vicinity of a black hole by the specific angular momentum. Using two-dimensional hydrodynamic simulations in cylindrical geometry, we present various regimes in which the accretion flows behave distinctly differently. When the flow has a small angular momentum $(\lambda\lsim\lambda_b)$, most of the material is accreted into the black hole forming a quasi-spherical flow or a simple disk-like structure around it. When the flow has a large angular momentum (typically, larger than the marginally bound value, $\lambda\gsim\lambda_{mb}$), almost no accretion into the …

PhysicsAngular momentumAstrophysics::High Energy Astrophysical PhenomenaAstrophysics (astro-ph)High Energy Physics::PhenomenologyFOS: Physical sciencesZero-point energyAstronomy and AstrophysicsAstrophysicsAstrophysicsLambdaSpecific relative angular momentumVortexPhysics::Fluid DynamicsBlack holeSpace and Planetary ScienceInviscid flowAdiabatic processThe Astrophysical Journal
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Quantum Monte Carlo methods

2005

Introduction In most of the discussion presented so far in this book, the quantum character of atoms and electrons has been ignored. The Ising spin models have been an exception, but since the Ising Hamiltonian is diagonal (in the absence of a transverse magnetic field), all energy eigenvalues are known and the Monte Carlo sampling can be carried out just as in the case of classical statistical mechanics. Furthermore, the physical properties are in accord with the third law of thermodynamics for Ising-type Hamiltonians (e.g. entropy S and specific heat vanish for temperature T → 0, etc.) in contrast to the other truly classical models dealt with in previous chapters (e.g. classical Heisenbe…

PhysicsEntropy (statistical thermodynamics)Quantum Monte CarloMonte Carlo methodZero-point energyClassical fluidsStatistical mechanicsHybrid Monte Carlosymbols.namesakeQuantum mechanicsDynamic Monte Carlo methodsymbolsMonte Carlo method in statistical physicsIsing modelKinetic Monte CarloStatistical physicsQuasi-Monte Carlo methodHamiltonian (quantum mechanics)Monte Carlo molecular modelingSpin-½
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van der Waals Interaction Energy Between Two Atoms Moving With Uniform Acceleration

2013

We consider the interatomic van der Waals interaction energy between two neutral ground-state atoms moving in the vacuum space with the same uniform acceleration. We assume the acceleration orthogonal to their separation, so that their mutual distance remains constant. Using a model for the van der Waals dispersion interaction based on the interaction between the instantaneous atomic dipole moments, which are induced and correlated by the zero-point field fluctuations, we evaluate the interaction energy between the two accelerating atoms in terms of quantities expressed in the laboratory reference frame. We find that the dependence of the van der Waals interaction between the atoms from the…

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsQuantum PhysicsField (physics)Zero-point energyFOS: Physical sciencesCasimir-Polder interactionInteraction energyGeneral Relativity and Quantum Cosmology (gr-qc)van der Waals forceGeneral Relativity and Quantum CosmologyCasimir effectDipolesymbols.namesakeUnruh effectHigh Energy Physics - Theory (hep-th)Quantum mechanicssymbolsUnruh effectvan der Waals forceAtomic physicsQuantum Physics (quant-ph)Energy (signal processing)
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The momentum and the angular momentum of the Universe revisited. Some preliminary results

2007

We consider the question of properly defining energy and momenta for non asymptotic Minkowskian spaces in general relativity. Only those of these spaces which have zero energy, zero linear 3-momentum, and zero intrinsic angular momentum would be candidates to creatable universes, that is, to universes which could have arisen from a vacuum quantum fluctuation. Given a universe, we completely characterize the family of coordinate systems in which it would make sense saying that this universe can be a creatable universe.

PhysicsHistoryAngular momentumGeneral relativitymedia_common.quotation_subjectZero-point energyUniverseComputer Science ApplicationsEducationMomentumTheoretical physicsClassical mechanicsTotal angular momentum quantum numberAngular momentum couplingZero-energy universemedia_commonJournal of Physics: Conference Series
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The zero-point energy for rotation

1978

The Gaussian overlap approach (GOA) becomes inappropriate for describing the rotation of weakly deformed systems. A modification is proposed which allows to maintain the GOA for small deformations. The zero-point energy subtraction, derived from it, provides a simple and reliable approximation for angular momentum projection. It becomes obvious, however, that the projection complicates the equations which determine the motion along the deformation path. These effects are studied in some simple models and the results are condensed into a simple interpolation formula for the total zero-point energy.

PhysicsNuclear and High Energy PhysicsAngular momentumsymbols.namesakeClassical mechanicsSimple (abstract algebra)GaussianZero (complex analysis)symbolsZero-point energyRotation (mathematics)Projection (linear algebra)Energy (signal processing)Zeitschrift f�r Physik A
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Systematics of parton-medium interaction from RHIC to LHC

2011

Despite a wealth of experimental data for high-P_T processes in heavy-ion collisions, discriminating between different models of hard parton-medium interactions has been difficult. A key reason is that the pQCD parton spectrum at RHIC is falling so steeply that distinguishing even a moderate shift in parton energy from complete parton absorption is essentially impossible. In essence, energy loss models are effectively only probed in the vicinity of zero energy loss and, as a result, at RHIC energies only the pathlength dependence of energy loss offers some discriminating power. At LHC however, this is no longer the case: Due to the much flatter shape of the parton p_T spectra originating fr…

PhysicsNuclear and High Energy PhysicsEnergy lossLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesZero-point energyParton01 natural sciencesSpectral lineModel dynamicsNuclear physicsStrange matterHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsAbsorption (electromagnetic radiation)Nuclear Experiment
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Effect of zero-point motion on the superconducting transition temperature of PdH(D)

1984

Using self-consistent density functional formalism we show that the electronic structure of PdH(D) is influenced by the zero-point vibration of hydrogen and deuterium. This quantum effect makes a small but significant contribution to the superconducting transition temperature ${T}_{c}$ of PdH(D). The reverse isotope effect on ${T}_{c}$ is found to be dominated by the changes in the force constants between PdH and PdD.

SuperconductivityPhysicsDeuteriumCondensed matter physicsTransition temperatureExcited stateKinetic isotope effectZero-point energyElectronic structureQuantum Hall effectAtomic physicsPhysical Review B
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Convergent transformations into a normal form in analytic Hamiltonian systems with two degrees of freedom on the zero energy surface near degenerate …

2004

We study an analytic Hamiltonian system with two degrees of freedom, having the origin as an elliptic singularity. We assume that the full Birkhoff normal form exists and is divisible by its quadratic part, being indefinite. We show that under the Bruno condition and under the restriction to the zero energy surface, a real analytic transformation into a normal form exists. Such a normal form coincides with the restriction of the Birkhoff normal form to the zero energy surface up to an order as large as we want.

Surface (mathematics)Quadratic equationSingularityApplied MathematicsGeneral MathematicsDegenerate energy levelsMathematical analysisZero-point energyOrder (ring theory)Gravitational singularityMathematical physicsHamiltonian systemMathematicsErgodic Theory and Dynamical Systems
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Quantum memories with zero-energy Majorana modes and experimental constraints

2016

In this work we address the problem of realizing a reliable quantum memory based on zero-energy Majorana modes in the presence of experimental constraints on the operations aimed at recovering the information. In particular, we characterize the best recovery operation acting only on the zero-energy Majorana modes and the memory fidelity that can be therewith achieved. In order to understand the effect of such restriction, we discuss two examples of noise models acting on the topological system and compare the amount of information that can be recovered by accessing either the whole system, or the zero-modes only, with particular attention to the scaling with the size of the system and the e…

media_common.quotation_subjectZero-point energyMarkov processFidelityFOS: Physical sciences02 engineering and technologyTopology01 natural sciencessymbols.namesakeTheoretical physics0103 physical sciencesThermal010306 general physicsScalingQuantummedia_commonPhysicsQuantum PhysicsTOPOLOGICAL INSULATORS; ONE 2ND; FERMIONS; SUPERCONDUCTOR; COMPUTATION; SUPERFLUIDS; ANYONS021001 nanoscience & nanotechnologyAtomic and Molecular Physics and OpticsCondensed Matter - Other Condensed MatterMAJORANAsymbols0210 nano-technologyHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Other Condensed Matter (cond-mat.other)
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On the convergence of zero-point vibrational corrections to nuclear shieldings and shielding anisotropies towards the complete basis set limit in wat…

2016

The method and basis set dependence of zero-point vibrational corrections (ZPVCs) to nuclear magnetic resonance shielding constants and anisotropies has been investigated using water as a test system. A systematic comparison has been made using the Hartree–Fock, second-order Møller–Plesset perturbation theory (MP2), coupled cluster singles and doubles (CCSD), coupled cluster singles and doubles with perturbative triples corrections (CCSD(T)) and Kohn–Sham density functional theory with the B3LYP exchange-correlation functional methods in combination with the second-order vibrational perturbation theory (VPT2) approach for the vibrational corrections. As basis sets, the correlation consisten…

waterBiophysicsZero-point energyzero-point vibrational correctionMonotonic function010402 general chemistry01 natural sciencesQuantum mechanics0103 physical sciencesPhysics::Atomic and Molecular ClustersCCSD(T)Limit (mathematics)complete basis set limitPhysics::Chemical PhysicsPhysical and Theoretical ChemistryMolecular BiologyBasis setPhysics010304 chemical physicsBasis (linear algebra)Condensed Matter PhysicsNMR shielding constant0104 chemical sciencesCoupled clusterDensity functional theoryPerturbation theory (quantum mechanics)Molecular Physics
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